magnetic tunnel junctions for magnetic random access memory applications m. guth), g. schmerber, a....

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Magnetic tunnel junctions f or magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

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Page 1: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

Magnetic tunnel junctions for magnetic random access memory

applications

M. Guth), G. Schmerber, A. DiniaFrance 2002

Page 2: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

Advantage

MRAM have a longevity because of the very important number of reader/write cycles that they can bear.( The write time is not clearly determined; it is reasonable that this time will be lower than 10 ns for addressing bit-memory. )

The commercial memories are in a constant competition for reducing bit memory size and increasing density.( MRAM can satisfy this target because of the bit-memory matrix addressing structure. )

Power consumption is 1 to 2 times lower than the traditional DRAMmemories.

Page 3: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

Comparison of a number of characteristics for different Random Access Memories

Page 4: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

These two states will constitute the two binary states in MRAM devices.

Page 5: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

MRAM’s matrix of MTJ cells and the magnetic field induced by the current flow in a bit line or a word line.

Page 6: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

barrier ( aluminum oxide ) most commonly used

Oxide has a high gap value and the resistance increases quickly by reducing the junction size, and will give resistance values not compatible with electronic devices.

Page 7: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

Si substrate

buffer layer Fe 6nm/Cu 30nm

CoFe 1.8nm/Ru 0.8nm/CoFe 3nm (AAF)

ZnS 2nm

CoFe 1nm

Fe 4nm / Cu 10nm / Ru 3nm

Page 8: Magnetic tunnel junctions for magnetic random access memory applications M. Guth), G. Schmerber, A. Dinia France 2002

I–V measurement for the 10× 10 mm2 patterned junction composed of Fe 6 nm Cu 30 nm CoFe 1.8 n

m Ru 0.8 nm CoFe 3 nm ZnS 2 nm CoFe 1 nm Fe 4 nm Cu 10nm Ru 3nm performed at room temperature. Circles correspond to the measured data and the full line corresponds to Brinkman's fit. The inset represents the dynamic conductance (d I/dV) from the I–V measurement at room temperature for parallel (gray line) and ant parallel (black line) orientation.